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標(biāo)題: Titlebook: Electron Correlation in New Materials and Nanosystems; Kurt Scharnberg,Sergei Kruchinin Conference proceedings 20071st edition Springer Sc [打印本頁(yè)]

作者: 退縮    時(shí)間: 2025-3-21 17:55
書(shū)目名稱(chēng)Electron Correlation in New Materials and Nanosystems影響因子(影響力)




書(shū)目名稱(chēng)Electron Correlation in New Materials and Nanosystems影響因子(影響力)學(xué)科排名




書(shū)目名稱(chēng)Electron Correlation in New Materials and Nanosystems網(wǎng)絡(luò)公開(kāi)度




書(shū)目名稱(chēng)Electron Correlation in New Materials and Nanosystems網(wǎng)絡(luò)公開(kāi)度學(xué)科排名




書(shū)目名稱(chēng)Electron Correlation in New Materials and Nanosystems被引頻次




書(shū)目名稱(chēng)Electron Correlation in New Materials and Nanosystems被引頻次學(xué)科排名




書(shū)目名稱(chēng)Electron Correlation in New Materials and Nanosystems年度引用




書(shū)目名稱(chēng)Electron Correlation in New Materials and Nanosystems年度引用學(xué)科排名




書(shū)目名稱(chēng)Electron Correlation in New Materials and Nanosystems讀者反饋




書(shū)目名稱(chēng)Electron Correlation in New Materials and Nanosystems讀者反饋學(xué)科排名





作者: Conduit    時(shí)間: 2025-3-21 21:44

作者: freight    時(shí)間: 2025-3-22 01:06
https://doi.org/10.1007/978-1-4842-2271-3down the source of this unacceptable result we consider the normal state. The elementary results for scattering off a hard sphere, including the result that even an infinitely strong .-function potential does not lead to scattering at all in systems of two and more dimensions, are recovered only whe
作者: 神圣不可    時(shí)間: 2025-3-22 07:41

作者: mechanical    時(shí)間: 2025-3-22 11:35
II.1 Magnesium diboride and the two-band scenariohe superconducting gap is estimated to be 2⊿/k.T. = 4.5, indicating that the superconductivity in Y.C. can be described by s-wave strong coupling regime. From specific heat in various magnetic fields, the upper critical field H.(0) is estimated to be 24.7 T.
作者: 天真    時(shí)間: 2025-3-22 14:18
II.2 Cuprate and other unconventional superconductorsdown the source of this unacceptable result we consider the normal state. The elementary results for scattering off a hard sphere, including the result that even an infinitely strong .-function potential does not lead to scattering at all in systems of two and more dimensions, are recovered only whe
作者: 天真    時(shí)間: 2025-3-22 17:29

作者: 沙發(fā)    時(shí)間: 2025-3-22 23:44
Conference proceedings 20071st editionials studied, strong electronic correlations provide a link between these two phenomena which were long thought to be highly antagonistic. Both the progress in our understanding of fundamental physical processes and the advances made towards the development of devices are reported here. The material
作者: reptile    時(shí)間: 2025-3-23 02:44

作者: 強(qiáng)制性    時(shí)間: 2025-3-23 06:17

作者: 逗留    時(shí)間: 2025-3-23 09:50

作者: 常到    時(shí)間: 2025-3-23 17:14
Raymond B. Seymour,Gerald S. Kirshenbauming of .- and .-wave symmetry of the superconducting order parameter in order to describe orthorhombic superconductors. We compare our calculations with new experimental data on fully untwinned YBa.Cu.O. and find good agreement. Our results are in contrast to earlier interpretations on the in-plane anisotropy in terms of stripes.
作者: Junction    時(shí)間: 2025-3-23 18:32

作者: GLOOM    時(shí)間: 2025-3-24 00:34
II.1 Magnesium diboride and the two-band scenarioa path integral approach. A definition of the critical level spacing of the two-gap superconductivity is also presented, and we discuss condensation energy and parity gap of the two-gap superconductivity in relation to the size dependence of those properties with two bulk gaps and effective pair scattering process between two sublevels.
作者: Cardiac-Output    時(shí)間: 2025-3-24 02:43

作者: Spartan    時(shí)間: 2025-3-24 08:57

作者: LIMIT    時(shí)間: 2025-3-24 10:55
G. Geiser,H. Foysi,W. Schr?der,M. Meinkeed with the change of the Fermi surface dimensionality of one of the superlattice subbands. The case of light element diborides where Mg is substituted for Al in AlB. and its similarity with intercalated graphite compounds is discussed.
作者: Accomplish    時(shí)間: 2025-3-24 16:08
SQL Server In-Memory Technologiesspin response in the coexisting DDW and d..-..-wave superconducting (DSC) states and discuss the peculiar features of the resonance peak dispersion. Furthermore, we investigate the infuence of various tight-binding parameters and the orthorhombic distortions on the robustness of the features discussed.
作者: CIS    時(shí)間: 2025-3-24 19:31
Toshiki Iwasaki,Masahiro Sawadathe non-ballistic (not spectral) regime of current flow in the nanocontacts. Thus, the current induced magnetoconductance effects in multilayered N–F structures (nanopillars) extensively studied in the recent literature have much more general character and can be stimulated by elastic electron scattering at single N–F interfaces.
作者: MUT    時(shí)間: 2025-3-25 02:03
MAGNETIC UNIPOLAR FEATURES IN CONDUCTIVITY OF POINT CONTACTS BETWEEN NORMAL AND FERROMAGNETIC D-METAthe non-ballistic (not spectral) regime of current flow in the nanocontacts. Thus, the current induced magnetoconductance effects in multilayered N–F structures (nanopillars) extensively studied in the recent literature have much more general character and can be stimulated by elastic electron scattering at single N–F interfaces.
作者: acclimate    時(shí)間: 2025-3-25 06:15
ELECTRON-ELECTRON INTERACTION IN CARBON NANOSTRUCTURESfor investigation. We found that λ. = 0.2 for arc-MWNTs (before and after bromination treatment); λ. = 0.1 for pyrolytic graphite; λ. >0 for c-MWNTs. We conclude that the curvature of graphene layers in carbon nanostructures leads to the increase of the electron-electron interaction constant λ..
作者: Malfunction    時(shí)間: 2025-3-25 09:58
II.1 Magnesium diboride and the two-band scenarioed with the change of the Fermi surface dimensionality of one of the superlattice subbands. The case of light element diborides where Mg is substituted for Al in AlB. and its similarity with intercalated graphite compounds is discussed.
作者: Exclude    時(shí)間: 2025-3-25 15:03
II.2 Cuprate and other unconventional superconductorsspin response in the coexisting DDW and d..-..-wave superconducting (DSC) states and discuss the peculiar features of the resonance peak dispersion. Furthermore, we investigate the infuence of various tight-binding parameters and the orthorhombic distortions on the robustness of the features discussed.
作者: Gourmet    時(shí)間: 2025-3-25 19:36

作者: 貪心    時(shí)間: 2025-3-25 22:47

作者: Respond    時(shí)間: 2025-3-26 00:19
NANOSCALE STUDIES ON METAL-ORGANIC INTERFACESeing accessed in the BEEM experiment, since the measured currents are larger than a purely tunneling contribution. Our results are consistent with previously published results on a similar molecule. Implications for device applications are briefly discussed.
作者: probate    時(shí)間: 2025-3-26 05:38
II.2 Cuprate and other unconventional superconductors taken, utilizing the phase-shifts inherent to the .-wave superconducting order parameter. This paper is intended to reflect the current status of experiments using high-T. and low-T. Josephson contacts.
作者: larder    時(shí)間: 2025-3-26 12:29

作者: 強(qiáng)有力    時(shí)間: 2025-3-26 13:25
https://doi.org/10.1007/3-540-29064-82-ethylhexyloxy)-p-phenylenevinylene (MEHPPV), and a metal-molecule interface Ag-terthiophene-Au, which are evaporated, spin-coated, and self assembled on an Au film respectively. All systems show spatially non-uniform carrier injection. Physical origins of the non-uniform carrier injection and its
作者: hysterectomy    時(shí)間: 2025-3-26 20:29
Michael Resch,Thomas B?nisch,Yoshiki Seoant λ. from the analysis of quantum correction to the magnetic susceptibility and the magnetoresistance was developed. Three types of carbon materials: arc-produced multiwalled carbon nanotubes (arc-MWNTs), CVD-produced catalytic multiwalled carbon nanotubes (c-MWNTs) and pyrolytic carbon were used
作者: 使更活躍    時(shí)間: 2025-3-27 00:57

作者: collateral    時(shí)間: 2025-3-27 03:53
Toshiki Iwasaki,Masahiro Sawadas voltage, ., on achieving of high current densities, 10. A/cm.. These features in . are observed when the electron flow is directed from the nonmagnetic metal into the ferromagnet and connected with magnetization excitations in the ferromagnet induced by the current. Applying an external magnetic f
作者: 眉毛    時(shí)間: 2025-3-27 07:40
Stefan Wesner,Sabine Roller,Harald Klimachrst, we review the present situation of the superconductivity in MgB., which can be interpreted in terms of BCS-type phonon-mediated pairing. In particular, we focus on the relationship between the superconductivity and the electronic structure in MgB. and two gap feature. Second, we review our pres
作者: 征服    時(shí)間: 2025-3-27 11:20
G. Geiser,H. Foysi,W. Schr?der,M. Meinkeantum condensates. This mechanism provides the Tc amplification in particular nanoscale material architectures like superlattices of metallic layers. The Feshbach resonance is reached by tuning the chemical potential to a Van Hove-Lifshitz singularity (vHs) in the electronic energy spectrum associat
作者: 控制    時(shí)間: 2025-3-27 15:51
Michael Resch,Xin Wang,Sabine Rolleret al., 2001; Golubov et al., 2002; Choi et al., 2002; Dahm, 2005). The two significantly different gaps exist on disconnected parts of the Fermi surface: a small gap (~2 meV) on the π bands and a large gap (~7 meV) residing on the σ bands. This leads to a number of peculiar consequences both in its
作者: Inexorable    時(shí)間: 2025-3-27 21:03
Xiaowei Xu,Jochen J?ger,Hans-Peter Kriegelexpressions for thermodynamic characteristics obtained. The dependence of superconducting gaps on Al doping are presented with the ⊿. crossing at . = 0.38. The calculated anisotropy coefficients for the MgB. critical magnetic fields agree with the experiment.
作者: 全能    時(shí)間: 2025-3-28 01:28
,Change-Coaching für High Performer,orresponding to a nanosize two-gap superconductivity is presented, and the partition function of the nanosize system is analytically derived by using a path integral approach. A definition of the critical level spacing of the two-gap superconductivity is also presented, and we discuss condensation e
作者: 小教堂    時(shí)間: 2025-3-28 04:01

作者: bypass    時(shí)間: 2025-3-28 10:00
https://doi.org/10.1007/978-94-011-0685-6d state are reviewed and discussed in the context of various theoretical frameworks. The increase observed in overdoped samples is compatible with a BCS condensation, while the decrease seen in underdoped samples is not. The significance of the sign reversal at or near optimum doping is given specia
作者: 獨(dú)行者    時(shí)間: 2025-3-28 11:39

作者: Outspoken    時(shí)間: 2025-3-28 17:58

作者: 燒烤    時(shí)間: 2025-3-28 19:13
SQL Server In-Memory Technologiesd cuprates. In particular we analyze the structure of the dynamical spin susceptibility in the DDW phase at the antiferromagnetic wave vector . = (π, π). We find that similar to the superconducting state a resonance peak forms. However, away from . it shows nearly no dispersion. We also analyze the
作者: 銀版照相    時(shí)間: 2025-3-29 01:10

作者: 碎石頭    時(shí)間: 2025-3-29 03:29
SPH Variants on Multi-GPU Architectures these species. The effective exchange integrals (J) of several transition-metal oxides have been calculated by hybrid DFT methods. The ab initio results for the species are also mapped to the N-band Hubbard model.
作者: 移動(dòng)    時(shí)間: 2025-3-29 09:04
978-1-4020-5658-1Springer Science+Business Media B.V. 2007
作者: 說(shuō)不出    時(shí)間: 2025-3-29 13:07

作者: 涂掉    時(shí)間: 2025-3-29 17:16
C. Lavalle,M. Rigol,J. Hub,A. Muramatsut ID versus source-drain voltage V. characteristics were observed at room temperature. We discuss this phenomenon in terms of the crossover from a diffusive conductance in bulk regime to a coherent one in the nanometer scale.
作者: 享樂(lè)主義者    時(shí)間: 2025-3-29 19:50

作者: FADE    時(shí)間: 2025-3-30 02:39

作者: 四指套    時(shí)間: 2025-3-30 08:02

作者: 多節(jié)    時(shí)間: 2025-3-30 09:36

作者: prostate-gland    時(shí)間: 2025-3-30 12:36

作者: 繁殖    時(shí)間: 2025-3-30 19:39
II.1 Magnesium diboride and the two-band scenarioexpressions for thermodynamic characteristics obtained. The dependence of superconducting gaps on Al doping are presented with the ⊿. crossing at . = 0.38. The calculated anisotropy coefficients for the MgB. critical magnetic fields agree with the experiment.
作者: trigger    時(shí)間: 2025-3-31 00:13
II.1 Magnesium diboride and the two-band scenariotion is derived according to the procedure of Richardson’s works. Parity gap and condensation energy of ultrasmall two-band superconducting grain are numerically obtained by solving the coupled equations. We discuss these properties in ultrasmall grain in relation to the correlation, interband interaction, and size dependence.
作者: 做方舟    時(shí)間: 2025-3-31 03:23

作者: Junction    時(shí)間: 2025-3-31 06:56
II.2 Cuprate and other unconventional superconductors these species. The effective exchange integrals (J) of several transition-metal oxides have been calculated by hybrid DFT methods. The ab initio results for the species are also mapped to the N-band Hubbard model.
作者: Exclude    時(shí)間: 2025-3-31 12:55
https://doi.org/10.1007/978-1-4020-5659-8Doping; Fulleren; Fullerene; Magnetic field; PED; PES; REM; STEM; Semiconductor; Superconductor; quantum dot; s
作者: 溫順    時(shí)間: 2025-3-31 17:05

作者: 不持續(xù)就爆    時(shí)間: 2025-3-31 21:22

作者: Aqueous-Humor    時(shí)間: 2025-3-31 22:08
TRANSPORT PROPERTIES OF FULLERENE NANODEVICESt ID versus source-drain voltage V. characteristics were observed at room temperature. We discuss this phenomenon in terms of the crossover from a diffusive conductance in bulk regime to a coherent one in the nanometer scale.
作者: 占卜者    時(shí)間: 2025-4-1 05:35
NANOSCALE STUDIES ON METAL-ORGANIC INTERFACES2-ethylhexyloxy)-p-phenylenevinylene (MEHPPV), and a metal-molecule interface Ag-terthiophene-Au, which are evaporated, spin-coated, and self assembled on an Au film respectively. All systems show spatially non-uniform carrier injection. Physical origins of the non-uniform carrier injection and its
作者: 終端    時(shí)間: 2025-4-1 09:30

作者: 一條卷發(fā)    時(shí)間: 2025-4-1 10:56
SINGLE-LEVEL MOLECULAR RECTIFIERis carried out. The analytic expressions for the combined sequential and tunnel current through the isolated reaction molecular level are derived with Coulomb interaction as well as an electron-vibration coupling taken into account. The combined hopping-tunnel model of the single-level molecular rec




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